The algebraic sum of the resolved parts of the forces in the given direction
The sum of the resolved parts of the forces in the given direction
The difference of the forces multiplied by the cosine of θ
The sum of the forces multiplied by the sine of θ
A. The algebraic sum of the resolved parts of the forces in the given direction
Angstrom
Light year
Micron
Milestone
Strain energy
Kinetic energy
Heat energy
Electrical energy
Lie on the same line
Meet at one point
Meet on the same plane
None of these
Two members with unknown forces of the frame
Three members with unknown forces of the frame
Four members with unknown forces of the frame
Three members with known forces of the frame
Inward
Outward
Towards front
Towards back
0.1 N-m
1 N-m
10 N-m
100 N-m
Potential energy
Kinetic energy
Power
None of these
P × OA
P × OB
P × OC
P × AC
The same as centre of gravity
The point of suspension
The point of application of the resultant of all the forces tending to cause a body to rotate about a certain axis
None of the above
Proportional to normal load between the surfaces
Dependent on the materials of contact surface
Proportional to velocity of sliding
Independent of the area of contact surfaces
The periodic time of a particle moving with simple harmonic motion is the time taken by a particle for one complete oscillation.
The periodic time of a particle moving with simple harmonic motion is directly proportional to its angular velocity.
The velocity of the particle moving with simple harmonic motion is zero at the mean position.
The acceleration of the particle moving with simple harmonic motion is maximum at the mean position.
Change its motion
Balance the forces, already acting on it
Give rise to the internal stresses in it
All of these
One-fourth of the total height above base
One-third of the total height above base
One-half of the total height above base
Three-eighth of the total height above the base
In the shaded area
In the hole
At O
None of these
Their algebraic sum is zero
Their lines of action are at equal distances
The algebraic sum of their moments about any point in their plane is zero
The algebraic sum of their moments about any point is equal to the moment of their resultant force about the same point.
W sinθ
W cosθ
W tanθ
W cotθ
0.5r
0.6 r
0.7 r
0.8 r
Reducing the problem of kinetics to equivalent statics problem
Determining stresses in the truss
Stability of floating bodies
Designing safe structures
m1/m2
m1. g. sin α
m1.m2/m1 + m2
m1. m2.g (1 + sin α)/(m1 + m2)
1 + m
1 - m
1 / m
m
Coplanar concurrent forces
Coplanar non-concurrent forces
Non-coplanar concurrent forces
None of these
IP = IG + Ah2
IP = IG - Ah2
IP = IG / Ah2
IP = Ah2 / IG
Newton's first law of motion
Newton's second law of motion
Newton's third law of motion
None of these
mr2/2
mr2/4
mr2/6
mr2/8
Kinetic friction
Limiting friction
Angle of repose
Coefficient of friction
Angular displacement
Angular velocity
Angular acceleration
All of these
Inelastic bodies
Elastic bodies
Neither elastic nor inelastic bodies
None of these
Coplanar force
Non-coplanar forces
Moment
Couple
Algebraic sum of the horizontal components of all the forces should be zero
Algebraic sum of the vertical components of all the forces should be zero
Algebraic sum of moments of all the forces about any point should be zero
All of the above
(2/3) Ml2
(1/3) Ml2
(3/4) Ml2
(1/12) Ml2